Calculation of Involved and Noninvolved Organs Doses in Carbon Therapy of Brain Tumor Using GEANT4 Simulation Toolkit

Introduction: This study used the GEANT4 Monte Carlo toolkit for radiation transport simulations in brain carbon therapy, incorporating a human phantom model to accurately assess dose delivery to targeted and non-targeted organs. Weight factors were employed to generate a Spread Out Bragg Peak (SOBP...

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Main Authors: Maria Ahmadi, Seyed Mohammad Motevalli, Payvand Taherparvar, Vahid zanganeh
Format: Article
Language:English
Published: Mashhad University of Medical Sciences 2024-10-01
Series:Iranian Journal of Medical Physics
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Online Access:https://ijmp.mums.ac.ir/article_25461_9ede827a90aee31a652da0f2845afe43.pdf
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author Maria Ahmadi
Seyed Mohammad Motevalli
Payvand Taherparvar
Vahid zanganeh
author_facet Maria Ahmadi
Seyed Mohammad Motevalli
Payvand Taherparvar
Vahid zanganeh
author_sort Maria Ahmadi
collection DOAJ
description Introduction: This study used the GEANT4 Monte Carlo toolkit for radiation transport simulations in brain carbon therapy, incorporating a human phantom model to accurately assess dose delivery to targeted and non-targeted organs. Weight factors were employed to generate a Spread Out Bragg Peak (SOBP).Material and Methods: The study used the ORNL-MIRD phantom to simulate carbon therapy for brain tumors, finding that the optimal energy range for carbon ions was 2420-2560 MeV to effectively cover the tumor. To achieve a homogeneous radiation dose, a Spread Out ragg Peak (SOBP) was generated using multiple Bragg peaks with specific intensity factors. Beam parameters were also evaluated per ICRU guidelines.Results: This study estimated the flux and dose distributions of secondary particles—protons, electrons, neutrons, alpha particles, and photons—in the brain tumor and surrounding tissues. We calculated the cumulative dose from both carbon ions and secondary particles, finding an absorbed dose ratio of 0.003 in healthy brain tissue compared to the tumor, with values of 4.8 × 10-4 for the skull and 2.6 × 10-5 for the thyroid. Notably, neutrons and photons can significantly increase energy transfer to distant organs, raising secondary cancer risk.Conclusion: The findings presented in this article demonstrated that the involvement of secondary particles in the dose received by both the brain and other organs remains minimal, as the highest absorbed dose was predominantly localized within the tumor.
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publisher Mashhad University of Medical Sciences
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spelling doaj-art-788723bd4e184942ad937972b34059422025-01-18T07:29:18ZengMashhad University of Medical SciencesIranian Journal of Medical Physics2345-36722024-10-0121528729410.22038/ijmp.2023.71006.225125461Calculation of Involved and Noninvolved Organs Doses in Carbon Therapy of Brain Tumor Using GEANT4 Simulation ToolkitMaria Ahmadi0Seyed Mohammad Motevalli1Payvand Taherparvar2Vahid zanganeh3Department of Nuclear Physics, Faculty of Science, University of Mazandaran P.O.Box 47415-416, Babolsar, IranDepartment of Nuclear Physics, Faculty of Science, University of Mazandaran, P. O. Box 47415-416, Babolsar, IranDepartment of Physics, Faculty of Science, University of Guilan, Rasht, IranGolestan university faculty of science, department of physics, Golestan, IranIntroduction: This study used the GEANT4 Monte Carlo toolkit for radiation transport simulations in brain carbon therapy, incorporating a human phantom model to accurately assess dose delivery to targeted and non-targeted organs. Weight factors were employed to generate a Spread Out Bragg Peak (SOBP).Material and Methods: The study used the ORNL-MIRD phantom to simulate carbon therapy for brain tumors, finding that the optimal energy range for carbon ions was 2420-2560 MeV to effectively cover the tumor. To achieve a homogeneous radiation dose, a Spread Out ragg Peak (SOBP) was generated using multiple Bragg peaks with specific intensity factors. Beam parameters were also evaluated per ICRU guidelines.Results: This study estimated the flux and dose distributions of secondary particles—protons, electrons, neutrons, alpha particles, and photons—in the brain tumor and surrounding tissues. We calculated the cumulative dose from both carbon ions and secondary particles, finding an absorbed dose ratio of 0.003 in healthy brain tissue compared to the tumor, with values of 4.8 × 10-4 for the skull and 2.6 × 10-5 for the thyroid. Notably, neutrons and photons can significantly increase energy transfer to distant organs, raising secondary cancer risk.Conclusion: The findings presented in this article demonstrated that the involvement of secondary particles in the dose received by both the brain and other organs remains minimal, as the highest absorbed dose was predominantly localized within the tumor.https://ijmp.mums.ac.ir/article_25461_9ede827a90aee31a652da0f2845afe43.pdfheavy ion radiotherapybrainmonte carlo simulation sobp
spellingShingle Maria Ahmadi
Seyed Mohammad Motevalli
Payvand Taherparvar
Vahid zanganeh
Calculation of Involved and Noninvolved Organs Doses in Carbon Therapy of Brain Tumor Using GEANT4 Simulation Toolkit
Iranian Journal of Medical Physics
heavy ion radiotherapy
brain
monte carlo simulation sobp
title Calculation of Involved and Noninvolved Organs Doses in Carbon Therapy of Brain Tumor Using GEANT4 Simulation Toolkit
title_full Calculation of Involved and Noninvolved Organs Doses in Carbon Therapy of Brain Tumor Using GEANT4 Simulation Toolkit
title_fullStr Calculation of Involved and Noninvolved Organs Doses in Carbon Therapy of Brain Tumor Using GEANT4 Simulation Toolkit
title_full_unstemmed Calculation of Involved and Noninvolved Organs Doses in Carbon Therapy of Brain Tumor Using GEANT4 Simulation Toolkit
title_short Calculation of Involved and Noninvolved Organs Doses in Carbon Therapy of Brain Tumor Using GEANT4 Simulation Toolkit
title_sort calculation of involved and noninvolved organs doses in carbon therapy of brain tumor using geant4 simulation toolkit
topic heavy ion radiotherapy
brain
monte carlo simulation sobp
url https://ijmp.mums.ac.ir/article_25461_9ede827a90aee31a652da0f2845afe43.pdf
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